Inertially-aided air data computer altitude

ABSTRACT

An air data computer configured to be installed on an aircraft includes an inertial sensor assembly having a plurality of accelerometers and a plurality of rate gyroscopes. The air data computer is configured to: determine a pressure altitude of the aircraft based on measured pressure of the airflow about the exterior of the aircraft; determine an estimated attitude of the aircraft based on rotational rate sensed by the plurality of rate gyroscopes; and determine a vertical acceleration of the aircraft based on the estimated attitude of the aircraft and the acceleration sensed by the plurality of accelerometers. The air data computer is further configured to blend the vertical acceleration and the pressure altitude using a complementary filter to produce a blended altitude rate that is output to consuming systems.

BACKGROUND

This disclosure relates generally to air data systems, and more particularly to air data systems that combine inertial sensor measurements and pneumatic pressure measurements for generating aircraft air data parameters.

Modern aircraft often incorporate air data systems that calculate air data outputs based on measured parameters collected from various sensors positioned about the aircraft. For instance, many air data systems utilize air data probes that measure pneumatic pressure of airflow about the aircraft exterior to generate aircraft air data outputs, such as angle of attack, calibrated airspeed, Mach number, altitude, altitude rate (i.e., aircraft vertical speed), or other air data parameters. Such air data parameters are then output to consuming systems, such as aircraft flight management systems, flight control systems, stall protection systems, and other consuming systems that utilize the air data parameters for operational control of the aircraft.

Often, air data systems generate an altitude rate output by differentiating the altitude parameter derived from the measured pressures. Because such numerical differentiation techniques typically amplify the high frequency components of the pressure-based measurements, the resulting altitude rate is often processed through low-pass filters that pass signals with frequencies lower than a cutoff frequency and attenuate signals with frequencies higher than the cutoff frequency. Such low-pass filtering techniques, however, typically rely on past data and introduce lag, thereby decreasing the dynamic response of the altitude rate output.

SUMMARY

In one example, an air data computer configured to be installed on an aircraft includes an inertial sensor assembly, an air data parameter module, an attitude determination module, and an altitude rate blending module. The inertial sensor assembly includes a plurality of accelerometers and a plurality of rate gyroscopes. The air data parameter module is configured to determine a pressure altitude of the aircraft based on measured pressure of airflow about an exterior of the aircraft. The attitude determination module is configured to determine an estimated attitude of the aircraft based on rotational rate sensed by the plurality of rate gyroscopes. The altitude rate blending module is configured to determine a vertical acceleration of the aircraft based on the estimated attitude of the aircraft and acceleration sensed by the plurality of accelerometers, blend the vertical acceleration and the pressure altitude using a complementary filter to produce a blended altitude rate, and output the blended altitude rate.

In another example, a method includes sensing acceleration of an air data computer configured to be installed on an aircraft along a plurality of axes via a plurality of accelerometers of an inertial sensor assembly of the air data computer. The method further includes sensing rotational rate of the air data computer along the plurality of axes via a plurality of rate gyroscopes of the inertial sensor assembly. The method further includes determining a pressure altitude of the aircraft based on measured pressure of airflow about an exterior of the aircraft, determining an estimated attitude of the aircraft based on the rotational rate sensed by the plurality of rate gyroscopes, and determining a vertical acceleration of the aircraft based on the estimated attitude of the aircraft and the acceleration sensed by the plurality of accelerometers. The method further includes blending the vertical acceleration and the pressure altitude using a complementary filter to produce a blended altitude rate, and outputting the blended altitude rate.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a schematic block diagram illustrating an example air data computer that utilizes air data parameters generated based on measured pressure inputs and acceleration sensed by an inertial sensor assembly to produce a blended altitude rate output.

FIG. 2 is a schematic block diagram illustrating further details of the inertial sensor compensation and correction module of FIG. 1 to produce error-corrected acceleration and angular rate outputs.

FIG. 3 is a schematic block diagram illustrating further details of the attitude determination module of FIG. 1 to determine a vehicle attitude using the error-corrected and compensated acceleration and angular rate outputs from the inertial sensor compensation and correction module.

FIG. 4 is a schematic block diagram illustrating further details of the Kalman estimator module of FIG. 1 to produce bias and scale factor error correction values that are utilized by the IMU to produce error-corrected acceleration and angular rate outputs.

FIG. 5 is a schematic block diagram illustrating details of the Kalman estimator module of FIG. 1 to produce an initial attitude quaternion representing an initial attitude of the IMU.

FIG. 6 is a schematic block diagram illustrating further details of the altitude rate blending module of FIG. 1 to produce a blended altitude rate output.

DETAILED DESCRIPTION

As described herein, an air data computer includes an inertial sensor assembly having a plurality of accelerometers and a plurality of rate gyroscopes. The air data computer determines aircraft altitude based on measured pressures of airflow about an exterior of the aircraft sensed by, e.g., a pitot-static probe or other pneumatic pressure sensors. Rather than determine aircraft altitude rate (i.e., vertical speed) based solely on the measured pressures, the air data computer blends vertical acceleration of the aircraft sensed by the plurality of accelerometers with the pressure-based altitude parameter using a complementary filter to produce a blended altitude rate parameter that is output to consuming systems. The complementary filter combines low frequency components of differentiated pressure altitude with high frequency components of integrated accelerometer-based vertical acceleration, thereby maintaining accuracy of the pressure-based measurements and increasing a bandwidth of the resulting altitude rate output via the high frequency accelerometer-based components. Moreover, an air data computer implementing techniques of this disclosure utilizes pressure-based air data parameters, such as true airspeed and angle of attack, to estimate bias and/or scale factor errors of the accelerometer and rate gyroscope outputs. The air data computer removes the estimated errors from the sensed rotational rate and acceleration parameters to produce error-corrected acceleration and rotational rate values, thereby increasing an accuracy of the accelerometer and rate gyroscope outputs. As such, an air data computer implementing techniques described herein combines inertial sensor measurements and pneumatic pressure measurements to both increase an accuracy of the inertial sensor outputs and to produce an altitude rate output having increased dynamic response.

FIG. 1 is a schematic block diagram illustrating air data computer 10 that utilizes pneumatic-based air data parameters generated by air data parameter module 11 and sensed rotational rate and acceleration to produce error-corrected body-axis accelerations 12, error-corrected body-axis angular rates 14, and blended aircraft altitude rate 15. As illustrated in FIG. 1, air data computer 10 includes inertial sensor assembly 16, inertial sensor compensation and correction module 18, attitude determination module 20, Kalman estimator module 22, and altitude rate blending module 23. Inertial sensor assembly 16 includes accelerometers 24A, 24B, and 24C, analog-to-digital converter 26, temperature sensors 28A, 28B, and 28C, analog-to-digital converter 30, rate gyroscopes 32A, 32B, and 32C, and analog-to-digital converter 34.

As illustrated, air data computer 10 receives measured static pressure P_(S), measured total pressure P_(t), measured alpha pressure P_(α1), and measured alpha pressure P_(α2) as inputs from, e.g., a pitot-static probe positioned at an exterior of the aircraft and having a barrel portion configured to extend into an oncoming airflow about the exterior of the aircraft. The pitot-static probe can have a plurality of pressure sensing ports including, e.g., a total pressure sensing port disposed at a tip of the barrel portion for use in sensing total pressure of the oncoming airflow, alpha pressure sensing ports disposed at a top and bottom of the barrel portion for use in sensing angle of attack, and a static pressure sensing port for use in sensing static pressure of the oncoming airflow. Each of the pressure sensing ports can be pneumatically connected to one or more pressure sensors that measure the corresponding pressures and provide an indication of the measured pressure to air data computer 10. Air data parameter module 11 utilizes measured pressures P_(S), P_(t), P_(α1), and P_(α2) to determine pneumatic-based air data parameters, including true airspeed (TAS) 36, angle of attack (AOA) 38, and pressure altitude 39, as is generally known in the art.

Accelerometers 24A, 24B, and 24C of inertial sensor assembly 16 form a 3-axis triad of accelerometers, each mounted (e.g., on a circuit board) and aligned to sense acceleration forces along one of three mutually-orthogonal axes. Rate gyroscopes 32A, 32B, and 32C are similarly mounted (e.g., on the same circuit board) and aligned to sense a rotational rate along one of three mutually-orthogonal axes (e.g., roll rate, pitch rate, and yaw rate). Temperature sensors 28A, 28B, and 28C are mounted (e.g., on the same circuit board) proximate accelerometers 24A-24C and rate gyroscopes 32A-32C to sense a temperature of an operational environment within inertial sensor assembly 16. For instance, temperature sensor 28A can be mounted proximate accelerometer 24A and rate gyroscope 32A to sense a temperature of an operational environment within inertial sensor assembly 16 proximate accelerometer 24A and rate gyroscope 32A. Temperature sensor 28B can be mounted proximate accelerometer 24B and rate gyroscope 32B to sense a temperature of an operational environment within inertial sensor assembly 16 proximate accelerometer 24B and rate gyroscope 32B. Temperature sensor 28C can be mounted proximate accelerometer 24C and rate gyroscope 32C to sense a temperature of an operational environment within inertial sensor assembly 16 proximate accelerometer 24C and rate gyroscope 32C. Any one or more of accelerometers 24A-24B, temperature sensors 28A-28C, and rate gyroscopes 32A-32C can be implemented as micro-electro-mechanical systems (MEMS). In some examples, temperature sensors 28A-28C can be thermo-resistive sensors.

As illustrated, inertial sensor assembly 16 further includes analog-to-digital (A-to-D) converters 26, 30, and 34. Each of A-to-D converters 26, 30, and 34 includes discrete and/or integrated logic circuitry to convert an analog signal input, such as a voltage, to a digital numerical representation proportional to a magnitude of the analog signal input. In operation, A-to-D converter 26 converts a voltage output from each of accelerometers 24A-24C to a digital numerical representation proportional to a magnitude of the voltage output from the respective one of accelerometers 24A-24C. A-to-D converter 30 converts a voltage output from each of temperature sensors 28A-28C to a digital numerical representation proportional to a magnitude of the voltage output from the respective one of temperature sensors 28A-28C. A-to-D converter 34 converts a voltage output from each of rate gyroscopes 32A-32C to a digital numerical representation proportional to a magnitude of the voltage output from the respective one or rate gyroscopes 32A-32C.

Each of inertial sensor compensation and correction module 18, attitude determination module 20, Kalman estimator module 22, and altitude rate blending module 23 can be implemented in hardware, software, or combinations of hardware and software. For example, air data computer 10 can include one or more processors and computer-readable memory encoded with instructions that, when executed by the one or more processors, cause air data computer 10 to operate in accordance with techniques described herein. Examples of the one or more processors include any one or more of a microprocessor, a controller, a digital signal processor (DSP), an application specific integrated circuit (ASIC), a field-programmable gate array (FPGA), or other equivalent discrete or integrated logic circuitry. Computer-readable memory of air data computer 10 can be configured to store information within air data computer 10 during operation. The computer-readable memory can be described, in some examples, as computer-readable storage media. In some examples, a computer-readable storage medium can include a non-transitory medium. The term “non-transitory” can indicate that the storage medium is not embodied in a carrier wave or a propagated signal. In certain examples, a non-transitory storage medium can store data that can, over time, change (e.g., in RAM or cache). Computer-readable memory of air data computer 10 can include volatile and non-volatile memories. Examples of volatile memories can include random access memories (RAM), dynamic random access memories (DRAM), static random access memories (SRAM), and other forms of volatile memories Examples of non-volatile memories can include magnetic hard discs, optical discs, floppy discs, flash memories, or forms of electrically programmable memories (EPROM) or electrically erasable and programmable (EEPROM) memories.

As illustrated in FIG. 1, the outputs of A-to-D converter 26, A-to-D converter 30, and A-to-D converter 34 are provided as inputs to inertial sensor compensation and correction module 18, which also receives Kalman scale factor and bias error corrections from Kalman estimator module 22. Inertial sensor compensation and correction module 18, in some examples, outputs body-axis angular rates 12 and body-axis accelerations 14 (i.e., error-corrected output values) via, e.g., a data bus or other communicative connection for use by an inertial navigation system or other consuming system. In other examples, body-axis angular rates 12 and body-axis accelerations 14 may not be output to consuming systems, but rather may be used internally by air data computer 10.

Body-axis angular rates 12 and body-axis accelerations 14 are provided by inertial sensor compensation and correction module 18 to Kalman estimator module 22 as inputs. Body-axis accelerations 14 are further provided by inertial sensor compensation and correction module 18 to altitude rate blending module 23 as inputs. Body-axis angular rates 12 are also provided by inertial sensor compensation and correction module 18 to attitude determination module 20 as inputs.

Attitude determination module 20 further receives tilt error correction values δq and initial attitude quaternion q^(C) _(init) from Kalman estimator module 22 and provides attitude information outputs to Kalman estimator module 22 and altitude rate blending module 23 in the form of attitude quaternion q^(C). Kalman estimator module 22 further receives true airspeed 36 and angle of attack 39 from air data parameter module 11, and provides Kalman scale factor and bias error corrections to inertial sensor compensation and correction module 18 for use in modifying inputs received from accelerometers 24A-24C and rate gyroscopes 32A-32C to produce error-corrected outputs: body-axis angular rates 12; and body-axis accelerations 14.

Altitude rate blending module 23 receives as inputs body-axis accelerations 14 from inertial sensor compensation and correction module 18, attitude quaternion q^(C) from attitude determination module 20, and pressure altitude 39 from air data parameter module 11. Altitude rate blending module 23 utilizes attitude information from attitude quaternion q^(C) and body-axis accelerations 14 to determine a vertical acceleration of the aircraft. Altitude rate blending module 23 blends the vertical acceleration with pressure altitude 39 using a complementary filter to produce blended aircraft altitude rate 15, as is further described below. Blended aircraft altitude rate 15 is output by air data computer 10 via an aircraft data bus or other communications network to consuming systems, such as an aircraft flight management system, an aircraft automatic flight control system, or other consuming systems, which utilize blended aircraft altitude rate 15 for operational control of the aircraft.

In operation, accelerometers 24A-24C and rate gyroscopes 32A-32C sense acceleration forces and rotational rates along the three mutually-orthogonal axes. Temperature sensors 28A-28C sense a temperature of an operational environment of accelerometers 24A-24C and rate gyroscopes 32A-32C, for example on one or more circuit boards within a housing of air data computer 10 that encloses components of air data computer 10. The outputs of each of accelerometers 24A-24C, temperature sensors 28A-28C, and rate gyroscopes 32A-32C are provided to inertial sensor compensation and correction module 18 via A-to-D converters 26, 30, and 34, illustrated in FIG. 1 as V_(A), V_(T), and V_(ω). That is, V_(A) represents a three-dimensional vector, each element of the vector corresponding to the output from one of accelerometers 24A, 24B, and 24C. Similarly, V_(T) represents a three-dimensional vector, each element corresponding to the output from one of temperature sensors 28A, 28B, and 28C. V_(ω) also represents a three-dimensional vector, each element of the vector corresponding to the output from one of rate gyroscopes 32A, 32B, and 32C.

Inertial sensor compensation and correction module 18 applies compensation and correction factors to adjust each of the inputs V_(A), V_(T), and V_(ω) to produce body-axis angular rates 12 and body-axis accelerations 14. Body-axis angular rates 12 and body-axis accelerations 14 each represent three-axis outputs of error-compensated and error-corrected output values corresponding to the adjusted inputs V_(A), V_(T), and V_(ω). As is further described below, inertial sensor compensation and correction module 18 applies compensation and correction factors to inputs V_(A), V_(T), and V_(ω) to adjust inputs V_(A), V_(T), and V_(ω) to compensate for sensor scale factor errors corresponding to an error in the slope of the sensor output over a temperature range, bias errors corresponding to a non-zero offset in the sensor output over the temperature range, non-linearity errors corresponding to non-linearity of the sensor output over the temperature range, and non-orthogonality errors corresponding to offsets in the mutual-orthogonality of the sensor installations along the three axes within inertial sensor assembly 16. Such temperature-dependent scale factor errors, temperature-dependent bias errors, non-linearity errors, and non-orthogonality errors can be considered deterministic in nature. As such, compensation and correction factors applied by inertial sensor compensation and correction module 18 to compensate sensor inputs V_(A), V_(T), and V_(ω) for the deterministic errors can be pre-determined during, e.g., a testing phase in a laboratory or manufacturing facility and stored in computer-readable memory of air data computer 10 for use by inertial sensor compensation and correction module 18 during operation.

Accordingly, inertial sensor compensation and correction module 18 applies compensation and correction factors to adjust sensor inputs V_(A), V_(T) and V_(ω) to compensate for deterministic errors, such as temperature dependent errors and sensor installation position and alignment errors. In addition, as illustrated in FIG. 1, inertial sensor compensation and correction module 18 receives Kalman scale factor and bias error correction values from Kalman estimator module 22 and also applies the Kalman scale factor and bias error correction values to sensor inputs V_(A), V_(T) and V_(ω) to correct for non-deterministic sensor errors, as is further described below.

Inertial sensor compensation and correction module 18 outputs the error-compensated and error-corrected sensor inputs V_(A), V_(T) and V_(ω) (i.e., compensated and corrected via application of the temperature-dependent scale factor error compensation values, the Kalman scale factor error correction values, the temperature-dependent bias error compensation values, the Kalman bias error correction values, the non-linearity error compensation values, and the non-orthogonality error compensation values) as body-axis angular rates 12 and body-axis accelerations 14. As such, body-axis angular rates 12 and body-axis accelerations 14 represent error-compensated and error-corrected output values of rate gyroscopes 32A-32C and accelerometers 24A-24C, respectively, after compensation for deterministic errors (e.g., temperature-dependent scale factor errors, temperature-dependent bias errors, sensor non-linearity errors, and non-orthogonality errors) and correction for non-deterministic scale factor and bias errors that may arise during operation of air data computer 10 (e.g., turn-on to turn-on bias and scale factor errors, vibration-related bias and scale factor errors, or other non-deterministic errors).

As illustrated in FIG. 1, Kalman estimator module 22 receives as inputs body-axis angular rates 12 and body-axis accelerations 14 from inertial sensor compensation and correction module 18, as well as true airspeed 36 and angle of attack 38 from air data parameter module 11. In addition, Kalman estimator module 22 receives attitude information corresponding to aircraft roll and pitch in the form of attitude quaternion q^(C) from attitude determination module 20.

As is further described below, attitude determination module 20 utilizes body-axis angular rates 12 to determine an attitude quaternion q^(C) corresponding to a coordinate transform between local level and body-axis roll and pitch of, e.g., an aircraft within which air data computer 10 is installed. The determined attitude quaternion q^(C) is provided to Kalman estimator module 22.

Kalman estimator module 22 utilizes attitude quaternion q^(C) determined by attitude determination module 20 as well as body-axis angular rates 12 and body-axis accelerations 14 to determine a change in an integrated body-axis acceleration over a relatively short time duration (e.g., 0.5 seconds, 1.0 second, or other time durations), as is further described below. Kalman estimator module 22 compares the determined change in the integrated body-axis acceleration over the time duration to a difference in the received true airspeed 36 over the same time duration to determine an airspeed difference value. Kalman estimator module 22 provides the airspeed difference value as input to an extended Kalman filter implemented by Kalman estimator module 22 to determine estimated scale factor errors and bias errors for each of accelerometers 24A-24C and rate gyroscopes 32A-32C. The estimated scale factor errors and bias errors for each of accelerometers 24A-24C and rate gyroscopes 32A-32C are provided to inertial sensor compensation and correction module 18 as Kalman scale factor error correction values and Kalman bias error correction values associated with each of accelerometers 24A-24C and rate gyroscopes 32A-32C.

Inertial sensor compensation module 18 applies the received Kalman scale factor error correction values and bias error correction values, the temperature-dependent scale factor and bias error compensation values, the non-linearity error compensation values, and the non-orthogonality error compensation values to each of the received inputs from accelerometers 24A-24C and rate gyroscopes 32A-32C to produce error-corrected body-axis angular rates 12 and body-axis accelerations 14. Accordingly, air data computer 10, implementing techniques of this disclosure, iteratively determines Kalman scale factor and bias error correction values that are applied to (e.g., subtracted from, added to, or otherwise applied to) sensed values from accelerometers 24A-24C and rate gyroscopes 32A-32C to correct for non-deterministic scale factor errors and bias errors that are unpredictable in nature. The compensation for deterministic errors (e.g., via the temperature-dependent scale factor and bias error compensation values, the non-linearity error compensation values, and the non-orthogonality error compensation values) as well as the non-deterministic errors (e.g., via the Kalman scale factor and bias error correction values) increases the accuracy of body-axis angular rates 12 and body-axis accelerations 14 that can be output from air data computer 10 to consuming systems and/or utilized internally by air data computer 10.

For instance, as illustrated in FIG. 1, altitude rate blending module 23 receives body-axis accelerations 14 as inputs. Altitude rate blending module 23 utilizes body-axis accelerations 14 as well as attitude quaternion q^(C) to determine a vertical acceleration of the aircraft that is blended with pressure altitude 39 using a complementary filter to produce blended aircraft altitude rate 15. As such, increased accuracy of body-axis accelerations 14 increases an accuracy of the aircraft vertical acceleration computations, thereby increasing an accuracy of blended aircraft altitude rate 15. As is further described below, the complementary filter of altitude rate blending module 23 combines low frequency components of differentiated pressure altitude 39 with high frequency components of integrated aircraft vertical acceleration, thereby increasing a bandwidth of blended altitude rate 15. As such, techniques of this disclosure enable air data computer 10 to increase an accuracy of body-axis angular rates 12 and body-axis accelerations 14 as well as to produce blended altitude rate 15 having increased dynamic response.

FIG. 2 is a schematic block diagram illustrating further details of inertial sensor compensation and correction module 18 of FIG. 1 to produce error-compensated body-axis angular rates 12 and body-axis accelerations 14. As illustrated in FIG. 2, inertial sensor compensation and correction module 18 includes temperature low-pass filter 40, accelerometer low-pass filter 42, rate gyroscope low-pass filter 44, temperature module 46, temperature averaging module 48, accelerometer thermal scale factor and bias module 50, rate gyroscope thermal scale factor and bias module 52, acceleration cluster module 54, body accelerations module 56, output body accelerations module 58, angular rate cluster module 60, body angular rates module 62, and output body angular rates module 64. As further illustrated, inertial sensor compensation and correction module 18 receives V_(T), V_(A), and V_(ω) as inputs from inertial sensor assembly 16 (FIG. 1). In addition, inertial sensor compensation and correction module 18 receives Kalman accelerometer scale factor and bias error correction values E_(K-A) and Kalman rate gyroscope scale factor and bias error correction values E_(K-G) from Kalman estimator module 22. Inertial sensor compensation and correction module 18 outputs body-axis accelerations 14 and body-axis angular rates 12 which, in some examples, are output via one or more communication data buses for use by a consuming system, such as an aircraft inertial navigation system, stability augmentation system, or other consuming system. In addition, inertial sensor compensation and correction module 18 provides compensated and corrected body-axis accelerations A_(comp-B) as input to Kalman estimator module 22 as well as compensated and corrected body-axis angular rates ω_(comp-B) as input to both Kalman estimator module 22 and attitude determination module 20. Kalman estimator module 22 provides tilt error correction values δq as input to attitude determination module 20.

Each of temperature low-pass filter 40, accelerometer low-pass filter 42, and rate gyroscope low-pass filter 44 are low-pass filters (e.g., Butterworth low-pass filters or other types of low-pass filters) implemented in hardware and/or software and configured to pass signals with frequencies lower than a cutoff frequency and attenuate signals with frequencies higher than the cutoff frequency. Each of temperature low-pass filter 40, accelerometer low-pass filter 42, and rate gyroscope low-pass filter 44 can be configured with a same or different cutoff frequency.

The output of temperature low-pass filter 40 is provided to temperature module 46, which in turn provides temperatures T(n) as outputs to each of accelerometer thermal scale factor and bias module 50 and rate gyroscope thermal scale factor and bias module 52. Accelerometer thermal scale factor and bias module 50 outputs temperature-dependent accelerometer scale factor and bias error compensation values A_(SF-B) to acceleration cluster module 54. Rate gyroscope thermal scale factor and bias module 52 outputs temperature-dependent rate gyroscope scale factor and bias error compensation values G_(SF-B) to angular rate cluster module 60. The combined operations of temperature module 46, temperature averaging module 48, accelerometer thermal scale factor and bias module 50, and rate gyroscope thermal scale factor and bias module 52 form temperature compensation operations that provide temperature compensation scale factor and bias error compensation values for application to (e.g., subtraction from) input values sensed by accelerometers 24A-24C and rate gyroscopes 32A-32C (FIG. 1).

Acceleration cluster module 54 receives the temperature compensation scale factor and bias error compensation values A_(SF-B) from accelerometer thermal scale factor and bias module 50 and applies the temperature-dependent accelerometer scale factor error compensation values and the temperature-dependent accelerometer bias error compensation values, as well as the accelerometer non-linearity error compensation values and the accelerometer non-orthogonality error compensation values (e.g., stored in computer-readable memory of air data computer 10) to produce compensated accelerometer values A_(comp-S) in the sensor axis that are provided to body accelerations module 56. Body accelerations module 56 receives the compensated sensor-axis accelerations A_(comp-S) from acceleration cluster module 54 and Kalman accelerometer scale factor and bias error correction values E_(K-A) from Kalman estimator module 22. Body accelerations module 56 converts the compensated sensor-axis accelerations A_(comp-S) to the aircraft (or other vehicle) body-axis and applies the Kalman accelerometer scale factor and bias error correction values E_(K-A) to produce compensated and corrected accelerometer values A_(comp-B) in the body-axis that are provided as input to both output body accelerations module 58 and Kalman estimator module 22. Output body accelerations module 58 bandwidth-limits the received compensated and corrected body-axis accelerations A_(comp-B) to produce body-axis accelerations 14. The combined operations of acceleration cluster module 54, body accelerations module 56 and output body accelerations module 58 form accelerometer compensation operations that apply both deterministic error compensation values (e.g., temperature-dependent accelerometer scale factor error compensation values, temperature-dependent accelerometer bias error compensation values, accelerometer non-linearity error compensation values, and accelerometer non-orthogonality error compensation values) and non-deterministic correction values (e.g., Kalman accelerometer scale factor error correction values and Kalman accelerometer bias error correction values) to produce body-axis accelerations 14 (i.e., accelerations along each of the three axes of accelerometers 24A-24C) that are error-compensation and error-corrected for both the deterministic and non-deterministic errors.

As further illustrated in FIG. 2, angular rate cluster module 60 receives the temperature compensation scale factor and bias error compensation values G_(SF-B) from rate gyroscope thermal scale factor and bias module 52 and applies the temperature-dependent rate gyroscope scale factor error compensation values and the temperature-dependent rate-gyroscope bias error compensation values, as well as the rate gyroscope non-linearity error compensation values and the rate gyroscope non-orthogonality error compensation values (e.g., stored in computer-readable memory of air data computer 10) to produce compensated angular rate values ω_(comp-S) in the sensor axis that are provided to body angular rates module 62. Body angular rates module 62 receives the compensated sensor-axis angular rate values ω_(comp-S) from angular rate cluster module 60 and Kalman rate gyroscope scale factor and bias error correction values E_(K-G) from Kalman estimator module 22. Body angular rates module 62 converts the compensated sensor-axis angular rates ω_(comp-S) to the aircraft (or other vehicle) body-axis and applies the Kalman rate gyroscope scale factor and bias error correction values E_(K-G) to produce compensated and corrected angular rate values ω_(comp-B) in the body-axis that are provided as input to output body angular rates module 64, Kalman estimator module 22, and attitude determination module 20. Output body angular rates module 64 bandwidth-limits the received compensated and corrected body-axis angular rates ω_(comp-B) to produce body-axis angular rates 12. The combined operations of angular rate cluster module 60, body angular rates module 62 and output body angular rates module 64 form rate gyroscope compensation operations that apply deterministic error compensation values (e.g., temperature-dependent rate gyroscope scale factor error compensation values, temperature-dependent rate gyroscope bias error compensation values, rate gyroscope non-linearity error compensation values, and rate gyroscope non-orthogonality error compensation values) and non-deterministic error-correction values (e.g., Kalman rate gyroscope scale factor error correction values and Kalman rate gyroscope bias error correction values) to produce body-axis angular rates 12 (i.e., angular rates in each of the three axes of rate gyroscopes 32A-32C) that are error-compensation and error-corrected to compensate and correct for both the deterministic and non-deterministic errors.

In operation, temperature module 46 receives low-pass filtered inputs V_(T) from low-pass filter 40 which represents a three-dimensional vector, each element corresponding to a filtered digital representation of a voltage output of one of temperature sensors 28A, 28B, and 28C. Temperature module 46 converts the voltage representation associated with each of temperature sensors 28A-28C to a separate temperature value using a polynomial curve-fit having coefficients selected during, e.g., a testing phase to fit an output of the respective temperature sensors 28A-28C to a reference temperature input. Temperature module 46 provides temperatures T(n) (i.e., three temperature values, each corresponding to one of temperature sensors 28A-28C) to temperature averaging module 48. Temperature averaging module produces an average temperature output for each of the received input temperatures T(n), such as by using a moving average (e.g., over 8 samples, 10 samples, or other number of samples) or other central tendency technique. Temperature averaging module 48 provides the average temperature associated with each of temperature sensors 28A-28C to each of accelerometer thermal scale factor and bias module 50 and rate gyroscope thermal scale factor and bias module 52.

Accelerometer thermal scale factor and bias module 50 determines a temperature-dependent accelerometer scale factor error compensation value and a temperature-dependent accelerometer bias error compensation value corresponding to each of accelerometers 24A-24C. For example, accelerometer thermal scale factor and bias module 50 can apply the average input temperature value for the one of temperature sensors 28A-28C that is associated with (e.g. mounted proximate) accelerometer 24A as input to a polynomial curve fit of temperature-dependent accelerometer scale factor errors corresponding to accelerometer 24A having coefficients determined during, e.g., a testing phase (e.g., in a laboratory or manufacturing phase). Accelerometer thermal scale factor and bias module 50 can similarly apply average input temperature values for each of temperature sensors 28B and 28C that are associated with accelerometers 24B and 24C as input to separate polynomial curve fits of temperature-dependent accelerometer scale factor errors corresponding to each of accelerometer 24B and 24C having coefficients determined during the testing and/or manufacturing phase. Accelerometer thermal scale factor and bias module 50 applies the average temperature input value for each of temperature sensors 28A-28C as input to polynomial curve fits of temperature-dependent bias errors corresponding to each of accelerometers 24A-24C (each of the polynomial curve fits having coefficients determined during the testing and/or manufacturing phase) to determine temperature-dependent bias error compensation values corresponding to each of accelerometers 24A-24C.

Rate gyroscope thermal scale factor and bias module 52 determines a temperature-dependent rate gyroscope scale factor error compensation value and a temperature-dependent rate gyroscope bias error compensation value corresponding to each of rate gyroscopes 32A-32C. For example, rate gyroscope thermal scale factor and bias module 52 can apply the average input temperature value for the one of temperature sensors 28A-28C that is associated with (e.g. mounted proximate) rate gyroscope 32A as input to a polynomial curve fit of temperature-dependent rate gyroscope scale factor errors corresponding to rate gyroscope 32A having coefficients determined during, e.g., a testing phase (e.g., in a laboratory or manufacturing phase). Rate gyroscope thermal scale factor and bias module 52 can similarly apply average input temperature values for each of temperature sensors 28B and 28C that are associated with rate gyroscopes 32B and 32C as input to separate polynomial curve fits of temperature-dependent rate gyroscope scale factor errors corresponding to each of rate gyroscopes 32B and 32C having coefficients determined during the testing and/or manufacturing phase. Rate gyroscope thermal scale factor and bias module 52 applies the average temperature input value for each of temperature sensors 28A-28C as input to polynomial curve fits of temperature-dependent bias errors corresponding to each of rate gyroscopes 32A-32C (each of the polynomial curve fits having coefficients determined during the testing and/or manufacturing phase) to determine temperature-dependent bias error compensation values corresponding to each of rate gyroscopes 32A-32C.

Acceleration cluster module 54 receives the temperature-dependent accelerometer scale factor error compensation values and the temperature-dependent accelerometer bias error compensation values from accelerometer thermal scale factor and bias module 50. In addition, acceleration cluster module 54 receives low-pass filtered inputs V_(A) from low-pass filter 42 which represents a three-dimensional vector, each element corresponding to a filtered digital representation of a voltage output of one of accelerometers 24A, 24B, and 24C. Acceleration cluster module 54 converts the voltage representation of each filtered input V_(A) to an acceleration value (e.g., in meters/second/second). In addition, acceleration cluster module 54 applies the received temperature-dependent accelerometer scale factor error compensation values corresponding to each of accelerometers 24A-24C to the inputs V_(A), such as by multiplying each of inputs V_(A) by the corresponding temperature-dependent accelerometer scale factor error compensation value. Acceleration cluster module 54 applies the received temperature-dependent accelerometer bias error compensation values corresponding to each of accelerometers 24A-24C to the inputs V_(A) via aggregation techniques (e.g., summing, subtracting, or other aggregation techniques). In addition, acceleration cluster module 54 applies (e.g., multiplies) the non-linearity error compensation values and the non-orthogonality error compensation values corresponding to each of accelerometers 24A-24C (e.g., determined during a testing and/or manufacturing phase and stored in computer-readable memory of air data computer 10) to the respective inputs V_(A) to produce compensated sensor-axis accelerations A_(comp-S). Sensor-axis accelerations A_(comp-S) therefore represent acceleration values associated with each of accelerometers 24A-24C in the sensor axis that have been compensated for deterministic errors corresponding to temperature-dependent scale factor and bias errors, sensor non-linearity errors, and non-orthogonality errors associated with a misalignment (i.e., non-mutually-orthogonal) of installation of accelerometers 24A-24C.

Body accelerations module 56 receives the compensated sensor-axis accelerations A_(comp-S) and converts the accelerations from the sensor coordinate frame to an aircraft (or other vehicle to which air data computer 10 is mounted) coordinate frame using a rotational matrix such as a direction cosine matrix having direction angles configured to transform the sensor coordinate frame to the aircraft body axis frame. In addition, body accelerations module 56 receives Kalman accelerometer scale factor and bias error correction values E_(K-A) from Kalman estimator module 22. As is further described below, Kalman accelerometer scale factor and bias error correction values E_(K-A) include scale factor error correction values and bias error correction values produced by an extended Kalman filter implemented by Kalman estimator module 22, each of the scale factor error correction values and bias error correction values corresponding to one of accelerometers 24A-24C. Body accelerations module 56 applies the Kalman accelerometer scale factor and bias error correction values E_(K-A) to the compensated acceleration values A_(comp-S) to produce compensated and corrected acceleration values A_(comp-B) in the body axis corresponding to each of accelerometers 24A-24C. The body axis can be defined by three mutually-orthogonal axes, a first of the three axes directed through the nose of the aircraft, a second of the three axes directed through a bottom of the aircraft toward the Earth when the aircraft is on-ground, and a third of the three axes directed orthogonally to the first axis and to the second axis and generally through a wing of the aircraft. Compensated and corrected acceleration values A_(comp-B) therefore represent body axis (e.g., aircraft body axis) accelerations corresponding to each of accelerometers 24A-24C that are compensated for deterministic errors (e.g., temperature-dependent scale factor and bias errors, sensor non-linearity errors, and non-orthogonality errors) and corrected for non-deterministic errors via Kalman scale factor and bias error correction values E_(K-A).

Body accelerations module 56 provides compensated and corrected acceleration values A_(comp-B) to output body accelerations module 58 and Kalman estimator module 22. Output body accelerations module 58 bandwidth-limits the output of compensated and corrected acceleration values A_(comp-B) via, e.g., an infinite impulse response (IIR) or other bandwidth-limiting filter to a defined bandwidth of a consuming system, such as an aircraft inertial navigation system. The bandwidth-limited acceleration values are provided by output body accelerations module 58 as body-axis accelerations 14.

As further illustrated in FIG. 2, temperature-dependent rate gyroscope scale factor and error compensation values and temperature-dependent rate gyroscope bias error compensation values determined by rate gyroscope thermal scale factor and bias module 52 are provided to angular rate cluster module 60 as input. In addition, angular rate cluster module 60 receives low-pass filtered inputs V_(ω) from low-pass filter 44 which represents a three-dimensional vector, each element corresponding to a filtered digital representation of a voltage output of one of rate gyroscopes 32A, 32B, and 32C. Angular rate cluster module 60 converts the voltage representation of each filtered input V_(ω) to an angular rate value (e.g., in meters/second). In addition, angular rate cluster module 60 applies the received temperature-dependent rate gyroscope scale factor error compensation values corresponding to each of rate gyroscopes 32A-32C to the inputs V_(ω), such as by multiplying each of inputs V_(ω) by the corresponding temperature-dependent rate gyroscope scale factor error compensation value. Angular rate cluster module 60 applies the received temperature-dependent rate gyroscope bias error compensation values corresponding to each of rate gyroscopes 32A-32C to the inputs V_(ω) via aggregation techniques (e.g., summing, subtracting, or other aggregation techniques). In addition, angular rate cluster module 50 applies (e.g., multiplies) the non-linearity error compensation values and the non-orthogonality error compensation values corresponding to each of rate gyroscopes 32A-32C (e.g., determined during a testing and/or manufacturing phase and stored in computer-readable memory of air data computer 10) to the respective inputs V_(ω) to produce compensated sensor-axis angular rates ω_(comp-S). Sensor-axis angular rates ω_(comp-S) therefore represent angular rate values associated with each of rate gyroscopes 32A-32C in the sensor axis that have been compensated for deterministic errors corresponding to temperature-dependent scale factor and bias errors, sensor non-linearity errors, and non-orthogonality errors associated with a misalignment (i.e., non-mutually-orthogonal) of installation of rate gyroscopes 32A-32C.

Body angular rates module 62 receives the compensated sensor-axis angular rate values ω_(comp-S) and converts the accelerations from the sensor coordinate frame to an aircraft (or other vehicle to which air data computer 10 is mounted) coordinate frame using a rotational matrix such as a direction cosine matrix having direction angles configured to transform the sensor coordinate frame to the aircraft body axis frame. In addition, body angular rates module 60 receives Kalman rate gyroscope scale factor and bias error correction values E_(K-G) from Kalman estimator module 22. As is further described below, Kalman rate gyroscope scale factor and bias error correction values E_(K-G) include scale factor error correction values and bias error correction values produced by the extended Kalman filter implemented by Kalman estimator module 22, each of the scale factor error correction values and bias error correction values corresponding to one of rate gyroscopes 32A-32C. Body angular rates module 62 applies the Kalman rate gyroscope scale factor and bias error correction values E_(K-G) to the compensated angular rate values ω_(comp-S) to produce compensated and corrected angular rate values ω_(comp-B) in the body axis corresponding to each of rate gyroscopes 32A-32C. As described above, the body axis can be defined by three mutually-orthogonal axes, a first of the three axes directed through the nose of the aircraft, a second of the three axes directed through a bottom of the aircraft toward the Earth when the aircraft is on-ground, and a third of the three axes directed orthogonally to the first axis and to the second axis and generally through a wing of the aircraft. Compensated and corrected angular rate values ω_(comp-B) therefore represent body axis (e.g., aircraft body axis) angular rates corresponding to each of rate gyroscopes 32A-32C that are compensated for deterministic errors (e.g., temperature-dependent scale factor and bias errors, sensor non-linearity errors, and non-orthogonality errors) as well as corrected for non-deterministic errors via Kalman scale factor and bias error correction values E_(K-G).

Body angular rates module 62 provides compensated and corrected angular rate values ω_(comp-B) to each of output body angular rates module 64, attitude determination module 20, and Kalman estimator module 22. Output body angular rates module 64 bandwidth-limits the output of compensated and corrected angular rate values ω_(comp-B) via, e.g., an infinite impulse response (IIR) or other bandwidth-limiting filter to a defined bandwidth of a consuming system, such as an aircraft inertial navigation system. The bandwidth-limited angular rate values are provided by output body angular rates module 64 as body-axis angular rates 12.

Accordingly, air data computer 10 implementing techniques described herein produces body-axis angular rates 12 and body-axis accelerations 14 that are compensated to correct for deterministic errors and corrected for non-deterministic errors. The techniques of this disclosure therefore increase an accuracy of outputs of air data computer 10 and enable air data computer 10 to adaptively modify such outputs (i.e., body-axis angular rates 12 and body-axis accelerations 14) to account for unpredictable errors that can arise during operation of air data computer 10 manifesting as sensor bias and scale factor errors.

FIG. 3 is a schematic block diagram illustrating further details of attitude determination module 20 of FIG. 1. As illustrated in FIG. 3, attitude determination module 20 includes body rate delta angles module 66 and propagate attitude quaternion module 68. Attitude determination module 20 receives compensated and corrected angular rate values ω_(comp-B) as inputs from inertial sensor compensation and correction module 18. Attitude determination module 20 outputs attitude quaternion q^(C) to Kalman estimator module 22 and altitude rate blending module 23.

As illustrated in FIG. 3, body rate delta angles module 66 receives compensated and corrected angular rate values ω_(comp-B) (i.e., compensated and corrected angular rates corresponding to the outputs from each of rate gyroscopes 32A-32C of FIG. 1) from inertial sensor compensation and correction module 18 (FIGS. 1 and 2) and provides angular displacement changes ψ_(ω) corresponding to each of rate gyroscopes 32A-32C as input to propagate attitude quaternion module 68. Propagate attitude quaternion module 68 receives angular displacement changes ψ_(ω) as input from body rate delta angles module 66 as well as initial attitude quaternion q^(C) _(init) and tilt error correction values δq from Kalman estimator module 22. Propagate attitude quaternion module 68 provides attitude quaternion q^(C) as input to each of Kalman estimator module 22 and altitude rate blending module 23.

In operation, body rate delta angles module 66 receives compensated and corrected angular rate values ω_(comp-B) corresponding to the compensated and corrected outputs of each of rate gyroscopes 32A-32C. Body rate delta angles module 66 integrates each of the compensated and corrected angular rate values ω_(comp-B) over a relatively short time interval, such as 0.001 seconds (i.e., corresponding to a 1 kHz sampling rate) to produce angular displacement changes ψ_(ω) corresponding to a change in angular displacement sensed by each of rate gyroscopes 32A-32C over the time interval.

Propagate attitude quaternion module 68 receives angular displacement changes ψ_(ω) from body rate delta angles module 66 and propagates the angular displacement changes over the time interval (e.g., 0.001 seconds) in quaternion form to produce attitude quaternion q^(C). Propagate attitude quaternion module 68 receives initial attitude quaternion q^(C) _(init) from Kalman estimator module 22 representing an initial attitude of air data computer 10, as is further described below. Propagate attitude quaternion module 68 propagates the received angular displacement changes ψ_(ω) over the time interval relative to the initial attitude quaternion q^(C) _(init) received from Kalman estimator module 22 (e.g., during a first execution of the attitude propagation operations). Propagate attitude quaternion module 68 applies tilt error correction values δq to the propagated attitude quaternion (e.g., via quaternion multiplication) to produce the error-corrected attitude quaternion q^(C).

As such, air data computer 10 implementing techniques of this disclosure determines vehicle attitude information represented by attitude quaternion q^(C) that is utilized by Kalman estimator module 22 to estimate sensor scale factor and bias errors that are provided as feedback to adjust and correct the sensed output values of accelerometers 24A-24C and gyroscopes 32A-32C.

FIG. 4 is a schematic block diagram illustrating further details of Kalman estimator module 22 to produce Kalman accelerometer scale factor and bias error correction values E_(K-A), Kalman rate gyroscope scale factor and bias error correction values E_(K-G), and tilt error correction values δq. As illustrated in FIG. 4, Kalman estimator module 22 includes check angle of attack (AOA) module 70, check true airspeed (TAS) module 72, reference velocity module 74, low-pass filter 76, low-pass filter 78, quaternion to direction-cosine module 80, low-pass filter 82, accelerometer root mean square (RMS) module 84, rate gyroscope RMS module 86, integrate reference velocity module 88, integrate Coriolis acceleration module 90, integrate direction-cosine module 92, integrate body accelerations module 94, velocity boost factor module 96, accelerometer boost factor module 98, rate gyroscope boost factor module 100, measurement matrix module 102, measurement vector module 104, state transition matrix module 106, process covariance noise matrix module 108, measurement covariance noise matrix module 110, Kalman filter module 112, tilt correction module 114, accelerometer bias and scale factor module 116, and rate gyroscope bias and scale factor module 118. As further illustrated, Kalman estimator module 22 receives true airspeed 36 and angle of attack 38 as input from air data parameter module 11, attitude quaternion q^(C) as input from attitude determination module 20, and compensated and corrected body-axis accelerations A_(comp-B) and compensated and corrected body-axis angular rates ω_(comp-B) as input from inertial sensor compensation and correction module 18. Kalman estimator module 22 outputs tilt error correction values δq, which are received as input by attitude determination module 20. In addition, Kalman estimator module 22 outputs accelerometer scale factor and bias error correction values E_(K-A), as well as rate gyroscope scale factor and bias error correction values E_(K-G). Accelerometer scale factor and bias error correction values E_(K-A) and rate gyroscope scale factor and bias error correction values E_(K-G) are received as input by inertial sensor compensation and correction module 18.

Check AOA module 70 receives angle of attack 38 as input, and outputs angle of attack α to reference velocity module 74. Check TAS module 72 receives true airspeed 36 as input and provides airspeed Va as output to reference velocity module 74 and low-pass filter 78, which passes the filtered reference velocity as input to velocity boost factor module 96. Compensated and corrected body-axis accelerations A_(comp-B) are received as input by both accelerometer RMS module 84 and integrate body accelerations module 94. Compensated and corrected body-axis angular rates ω_(comp-B) are received as input by both low-pass filter 82 and integrate Coriolis accelerations module 90. Attitude quaternion q^(C) is received as input by quaternion to direction-cosine module 80.

Reference velocity module 74 outputs body-axis reference velocity vector V_(ref), which is received as input by each of integrate reference velocity module 88, low-pass filter 76, and integrate Coriolis acceleration module 90. Low-pass filter 76 provides a filtered output of body-axis reference velocity vector V_(ref) to measurement vector module 104. Integrate reference velocity module 88 outputs integrated body-axis reference velocity vector ΣV_(ref) to measurement matrix module 102. Integrate Coriolis accelerations module 90 outputs integrated Coriolis acceleration ΣA_(C) to measurement vector module 104. Quaternion to direction-cosine module outputs direction-cosine matrix ΣC to integrate direction-cosine module 92, which provides integrated direction-cosine matrix ΣC as output to each of measurement matrix module 102, measurement vector module 104, and state transition matrix module 106. Integrate body accelerations module 94 outputs integrated compensated and corrected body-axis accelerations ΣA_(comp-B) to measurement vector module 104. Accelerometer RMS module 84 receives compensated and corrected body-axis accelerations A_(comp-B) from inertial sensor compensation and correction module 18, and outputs accelerations root mean square A_(RMS) to accelerometer boost factor module 98. Rate gyroscope RMS module 86 receives filtered compensated and corrected body-axis angular rates ω_(comp-B) from low-pass filter 82 and outputs angular rates root mean square ω_(RMS) to rate gyroscope boost factor module 100. Velocity boost factor module outputs velocity boost factor K_(V) to measurement covariance noise matrix module 110. Accelerometer boost factor module 98 outputs acceleration boost factor K_(A), which is received as input by each of process covariance noise matrix module 108 and measurement covariance noise matrix module 110. Rate gyroscope boost factor module 100 outputs angular rate boost factor K_(ω) to each of process covariance noise matrix module 108 and measurement covariance noise matrix module 110.

Measurement matrix module 102 outputs measurement matrix H to Kalman filter module 112. Measurement vector module 104 provides measurement vector y as input to Kalman filter module 112. State transition matrix module 106 outputs state transition matrix ϕ, which is received as input by Kalman filter module 112. Process covariance noise matrix module 108 outputs process covariance noise matrix Q, and measurement covariance noise matrix module 110 outputs measurement covariance noise matrix R. Each of process covariance noise matrix Q and measurement covariance noise matrix R is received as input by Kalman filter module 112.

Kalman filter module 112 outputs Kalman state vector X, which is received as input by each of tilt correction module 114, accelerometer bias and scale factor module 116, and rate gyroscope bias and scale factor module 118. Tilt correction module 114 outputs tilt error correction values δq to attitude determination module 20. Accelerometer bias and scale factor module 116 provides Kalman accelerometer scale factor and bias error correction values E_(K-A) as input to inertial sensor compensation and correction module 118. Rate gyroscope bias and scale factor module 118 outputs Kalman rate gyroscope scale factor and bias error correction values E_(K-G), which is received as input by inertial sensor compensation and correction module 18.

In operation, check AOA module 70 receives angle of attack 38 from, e.g., an aircraft air data system or other source. Check AOA module 70 determines whether the received angle of attack 38 is valid, such as by determining whether angle of attack 38 is within a predefined range of valid angles of attack and/or by accessing validity information included with angle of attack 38 (e.g., status field(s), bit(s), or other information indicating a validity status of angle of attack 38). Check AOA module 70 outputs angle of attack α as equal to the value (e.g., scalar value) of angle of attack 38 in response to determining that angle of attack 38 is valid. Check AOA module 70 outputs a as equal to a value of zero in response to determining that angle of attack 38 is invalid. Similarly, check TAS module 72 receives true airspeed 36 and determines a validity status of true airspeed 36 by determining whether true airspeed 36 is within a predefined range of valid true airspeeds and/or by accessing validity information included with true airspeed 36. Check TAS module 72 outputs airspeed Va as equal to the value (e.g., scalar value) of true airspeed 36 in response to determining that true airspeed 36 is valid. Check TAS module 72 outputs airspeed Va as equal to a value of zero in response to determining that true airspeed 36 is invalid.

Each of low-pass filters 76, 78, and 82 can be Butterworth filters, infinite impulse response filters, or other types of low-pass filters implemented in hardware and/or software and configured to pass signals with frequencies lower than a cutoff frequency and attenuate signals with frequencies higher than the cutoff frequency. Each of low-pass filters 76, 78, and 82 can be configured with a same or different cutoff frequency, and can be implemented using the same or different types of low-pass filters. Low-pass filter 78 receives airspeed Va and provides a filtered output of airspeed Va to velocity boost factor module 96.

Reference velocity module 74 utilizes angle of attack α and airspeed Va to produce body-axis reference velocity vector V_(ref). That is, reference velocity module 74 uses angle of attack α to convert the received scalar airspeed Va into a vector representation of the body frame velocity by attributing the airspeed Va to the forward and vertical body-axis velocity components using angle of attack α. Low-pass filter 76 receives body-axis reference velocity vector V_(ref) and provides a low-pass filtered output of body-axis reference velocity vector V_(ref) as input to measurement vector module 104. Quaternion to direction-cosine module 80 applies a transformation matrix to attitude quaternion q^(C) representing attitude information of air data computer 10 (e.g., pitch, roll, and yaw) to produce direction cosine matrix C representing the attitude information in direction-cosine form.

Each of integrate reference velocity module 88, integrate Coriolis acceleration module 90, integrate direction-cosine module 92, and integrate body accelerations module 94 integrate their respective inputs over a same time duration, such as 0.5 seconds, 1.0 seconds, or other time durations. That is, integrate reference velocity module 88 integrates body-axis reference velocity vector V_(ref) over the time duration using, e.g., trapezoidal integration or other numerical integration operations to produce integrated body-axis reference velocity vector ΣV_(ref) that is provided to measurement matrix module 102. Integrate Coriolis acceleration module 90 determines an instantaneous Coriolis acceleration force experienced by accelerometers 24A-24C (FIG. 1) as a cross product of compensated and corrected body-axis angular rates ω_(comp-B) and body-axis reference velocity vector V_(ref). Integrate Coriolis acceleration module 90 integrates the instantaneous Coriolis acceleration over the time duration (i.e., the same time duration utilized by integrate reference velocity module 88) to produce integrated Coriolis acceleration ΣA_(C). Integrate direction-cosine module 92 integrates direction-cosine matrix C over the same time duration to produce integrated direction-cosine matrix ΣC. Integrate body accelerations module 94 integrates compensated and corrected body-axis accelerations A_(comp-B) over the same time duration to produce integrated compensated and corrected body-axis accelerations ΣA_(comp-B).

Accelerometer RMS module 84 receives compensated and corrected body-axis accelerations A_(comp-B) and produces accelerations root mean square A_(RMS) by computing a root mean square of the received acceleration compensated and corrected body-axis accelerations A_(comp-B) or using other central tendency techniques. Rate gyroscopes RMS module 86 receives low-pass filtered compensated and corrected body-axis angular rates ω_(comp-B) from low-pass filter 82 and produces angular rates root mean square ω_(RMS) by computing a root mean square of the received filtered compensated and corrected body-axis angular rates ω_(comp-B) or using other central tendency techniques.

Velocity boost factor module 96 receives low-pass filtered airspeed Va from low-pass filter 78 and produces velocity boost factor K_(V) that is proportional to a rate of change of low-pass filtered airspeed Va with respect to time. That is, as the time rate of change of low-pass filtered airspeed Va increases, velocity boost factor K_(V) increases. As the time rate of change of low-pass filtered airspeed Va decreases, velocity boost factor K_(V) decreases. Similarly, accelerometer boost factor module 98 produces acceleration boost factor K_(A) that is proportional to a time rate of change of accelerations root mean square A_(RMS). Rate gyroscope boost factor module 100 produces angular rate boost factor K_(ω) that is proportional to a time rate of change of angular rates root mean square ω_(RMS).

Measurement matrix module 102, measurement vector module 104, state transition matrix module 106, process covariance noise matrix module 108, and measurement covariance noise matrix module 110 produce measurement matrix H, measurement vector y, state transition matrix ϕ, process covariance noise matrix Q, and measurement covariance noise matrix R, respectively, which are utilized during execution of an extended Kalman filter implemented by Kalman filter module 112 to produce Kalman state vector X that includes tilt error correction values δq, Kalman accelerometer scale factor and bias error correction values E_(K-A), and Kalman rate gyroscope scale factor and bias error correction values E_(K-G). Measurement matrix module 102 utilizes integrated reference velocity ΣV_(ref) and integrated direction-cosine matrix ΣC to produce measurement matrix H. Measurement vector module 104 utilizes low-pass filtered body-axis reference velocity vector V_(ref), integrated Coriolis acceleration ΣA_(C), integrated direction-cosine matrix ΣC, and integrated compensated and corrected body-axis accelerations ΣA_(comp-B) to generate measurement vector y. Measurement vector y represents a difference between a change in body-axis reference velocity vector V_(ref) over a time duration and a change in integrated compensated and corrected body-axis accelerations ΣA_(comp-B) over the same time duration with effects of integrated Coriolis acceleration ΣA_(C) and gravity removed (e.g., added, subtracted, or otherwise removed). For example, measurement vector module 104 can add the integrated Coriolis acceleration ΣA_(C) to the difference between the change in body-axis reference velocity vector V_(ref) and integrated compensated and corrected body-axis accelerations ΣA_(comp-B), and can subtract a value corresponding to the acceleration due to gravity (e.g., 9.8 meters/second/second) from the resulting sum.

State transition matrix module 106 utilizes integrated direction-cosine matrix ΣC to populate state transition matrix ϕ utilized by Kalman filter module 112 to propagate the Kalman state forward in time. Process covariance noise matrix module 108 utilizes acceleration boost factor K_(A) and angular rate boost factor K_(ω) to produce process noise covariance matrix Q that represents an estimate of uncertainty corresponding to process noise introduced by computational uncertainties or other process noise. Measurement covariance noise matrix module utilizes velocity boost factor K_(V), acceleration boost factor K_(A), and angular rate boost factor K_(ω) to produce measurement covariance noise matrix R that represents an estimate of uncertainty corresponding to sensor noise from accelerometers 24A-24C and rate gyroscopes 32A-32C (FIG. 1). Because each of velocity boost factor K_(V), acceleration boost factor K_(A), and angular rate boost factor K_(ω) are proportional to a rate of change of their respective inputs (i.e., low-pass filtered airspeed Va, accelerations root mean square A_(RMS), and angular rates root mean square ω_(RMS)), process covariance noise matrix module 108 and measurement covariance noise matrix module 110 effectively increase the effect of process covariance noise matrix Q and measurement covariance noise matrix R during execution of the extended Kalman filter implemented by Kalman filter module 112 during operational states corresponding to dynamic motion of air data computer 10.

Kalman filter module 112 implements an extended Kalman filter that utilizes measurement matrix H, measurement vector y, state transition matrix ϕ, process covariance matrix Q, and measurement covariance matrix R to produce Kalman state vector X. Kalman state vector X can be, e.g., a 16-element vector including (in any order): two tilt error correction values, one corresponding to pitch and the other corresponding to roll; three accelerometer bias error correction values, each corresponding to one of accelerometers 24A-24C; three accelerometer scale factor error correction values, each corresponding to one of accelerometers 24A-24C; three rate gyroscope bias error correction values, each corresponding to one of rate gyroscopes 32A-32C; three rate gyroscope scale factor error correction values, each corresponding to one of rate gyroscopes 32A-32C; and two transport rate error correction values corresponding to forward pitch rates experienced to maintain level flight while moving across the surface of the Earth.

Tilt correction module 114 utilizes the two tilt error correction values and the two transport rate error correction values to produce tilt error correction values δq, which are utilized by attitude determination module 20 during propagation of attitude quaternion q^(C), as is further described above. Accelerometer bias and scale factor module 116 applies (e.g., adds, subtracts, or otherwise applies) the three accelerometer bias error correction values to accelerometer bias error correction values determined during a previous execution (e.g., a previous iteration) of Kalman estimator module 22 to produce three updated accelerometer bias error correction values, each corresponding to one of accelerometers 24A-24C. Similarly, accelerometer bias and scale factor module 116 applies (e.g., adds, subtracts, or otherwise applies) the three accelerometer scale factor error correction values to accelerometer scale factor error correction values determined during a previous execution (e.g., a previous iteration) of Kalman estimator module 22 to produce three updated accelerometer scale factor error correction values, each corresponding to one of accelerometers 24A-24C. Accelerometer bias and scale factor module 116 outputs the three updated accelerometer bias error correction values and the three updated accelerometer scale factor error correction values as Kalman accelerometer scale factor and bias error correction values E_(K-A), which are received as input by inertial sensor compensation and correction module 18 and utilized during accelerometer error correction operations.

Rate gyroscope bias and scale factor module 118 applies (e.g., adds, subtracts, or otherwise applies) the three rate gyroscope bias error correction values of Kalman state vector X to rate gyroscope bias error correction values determined during a previous execution (e.g., a previous iteration) of Kalman estimator module 22 to produce three updated rate gyroscope bias error correction values, each corresponding to one of rate gyroscopes 32A-32C. Similarly, rate gyroscope bias and scale factor module 118 applies (e.g., adds, subtracts, or otherwise applies) the three rate gyroscope scale factor error correction values to rate gyroscope scale factor error correction values determined during a previous execution (e.g., a previous iteration) of Kalman estimator module 22 to produce three updated rate gyroscope scale factor error correction values, each corresponding to one of rate gyroscopes 32A-32C. Rate gyroscope bias and scale factor module 118 outputs the three updated rate gyroscope bias error correction values and the three updated rate gyroscope scale factor error correction values as Kalman rate gyroscope scale factor and bias error correction values E_(K-G), which are received as input by inertial sensor compensation and correction module 18 and utilized during rate gyroscope error correction operations.

Accordingly, air data computer 10 implementing Kalman estimator module 22, iteratively and adaptively determines scale factor and bias error correction values that are applied by inertial sensor compensation and correction module 18 to outputs of accelerometers 24A-24C and rate gyroscopes 32A-32C to produce error-compensated body-axis angular rates 12 and body-axis accelerations 14. As such, Kalman estimator module 22 can help to correct body-axis angular rates 12 and body-axis accelerations 14 for non-deterministic errors that can be unpredictable in nature.

FIG. 5 is a schematic block diagram illustrating details of Kalman estimator module 22 of FIG. 1 to produce initial attitude quaternion q^(C) _(init) representing an initial attitude of air data computer 10. That is, FIG. 5 illustrates details of Kalman estimator module 22 that are executed during an initialization phase of air data computer 10, such as after initial power-up, reset, or other initialization phases. In general, many modules and operations of Kalman estimator module 22 described with respect to the example of FIG. 5 are substantially similar to the modules and operations of Kalman estimator module 22 that were described above with respect to FIG. 4. For purposes of clarity and ease of discussion, the same reference numbers are used for like modules, and only differences in modules and operations are described below with respect to the example of FIG. 5.

As illustrated in FIG. 5, Kalman estimator module 22 includes update initial attitude estimate module 120 and update attitude module 122, which are implemented by Kalman estimator module 22 during initialization operations. In the example of FIG. 5, measurement matrix module 102 receives integrated direction-cosine matrix ΣC from integrate direction-cosine module 92 and produces measurement matrix H, which is passed to Kalman filter module 112. Kalman filter module 112 receives measurement vector y, and measurement covariance matrix R as input and executes an extended Kalman filter to produce Kalman state vector X_(C). Kalman state vector X_(C) is a three-element vector, the three elements corresponding to error correction values of the third row (i.e., pitch and roll components) of integrated direction-cosine matrix ΣC. Kalman filter module 112 outputs state vector X_(C) to update initial attitude estimate module 120, which applies (e.g., subtracts, adds, or otherwise applies) the error correction values from a previous execution (e.g., a previous iteration) of Kalman estimator module 22 to determine an updated initial attitude vector C_(3X). Update initial attitude estimate module 120 outputs updated initial attitude vector C_(3X) to measurement vector module 104, which applies (e.g., multiplies) updated initial attitude vector C_(3X) to measurement vector y to produce an updated measurement vector y. Kalman estimator module 22 iteratively executes measurement vector module 104, Kalman filter module 112, and update initial attitude estimate module 120 for a threshold time duration, such as 10 seconds or other threshold time durations, to iteratively determine and modify updated initial attitude vector C_(3X). Update initial attitude estimate module 120 provides updated initial attitude vector C_(3X) to update attitude module 122, which converts the attitude information of initial attitude vector C_(3X) to quaternion form and outputs initial attitude quaternion q^(C) _(init) to attitude determination module 20 for use during initialization operations of air data computer 10.

Accordingly, air data computer 10 implementing techniques of this disclosure, utilizes air data parameter values, such as true airspeed and angle of attack, to produce error-corrected angular rate and acceleration output values. Air data computer 10 determines vehicle attitude in the form of attitude quaternion q^(C) based on sensed acceleration and rotational position information received from accelerometers 24A-24C and gyroscopes 32A-32C. The air data parameter values are utilized by Kalman estimator module 22 to estimate sensor scale factor and bias errors that are provided as feedback to further adjust and correct the sensed output values of accelerometers 24A-24C and gyroscopes 32A-32C. Accordingly, the techniques described herein can increase an accuracy of computations and, in some examples, outputs of air data computer 10 (i.e., body-axis angular rates 12 and body-axis accelerations 14) by modifying the outputs to compensate for deterministic errors (e.g., temperature-dependent scale factor and bias errors, sensor non-linearity errors, and non-orthogonality errors) and correct for non-deterministic errors that can manifest as sensor scale factor and bias errors that arise during operation of (or between operations of) air data computer 10.

FIG. 6 is a schematic block diagram illustrating further details of altitude rate blending module 23 of FIG. 1 to produce blended altitude rate output 15. As illustrated in FIG. 6, altitude rate blending module 23 receives attitude quaternion q^(C) as input from attitude determination module 20 (FIGS. 1 and 3), body-axis accelerations 14 from inertial sensor compensation and correction module 18 (FIGS. 1 and 2), and pressure altitude 39 from air data parameter module 11 (FIG. 1). Altitude rate blending module 12 includes quaternion to direction-cosine module 124, body to local level accelerations module 126, and complementary filter 128. Complementary filter 128 includes differentiator 130 (indicated in Laplace transform space as S), integrator 132 (indicated in Laplace transform space as 1/S), low-pass filter (LPF) 134, and high-pass filter (HPF) 136.

Quaternion to direction-cosine module 124 applies a transformation matrix to attitude quaternion q^(C) representing attitude information of air data computer 10 (e.g., pitch, roll, and yaw) to produce direction-cosine matrix DC representing the attitude information in direction-cosine form. Body to local level accelerations module 126 receives direction-cosine matrix DC as input. In addition, body to local level accelerations module 126 receives body-axis accelerations 14 as input in vector form, each element of the vector corresponding to one of the accelerations sensed by accelerometers 24A-24C (FIG. 1) in the body-axis reference frame defined by three mutually-orthogonal axes, a first of the three axes directed through the nose of the aircraft, a second of the three axes directed through a bottom of the aircraft toward the Earth when the aircraft is on-ground, and a third of the three axes directed orthogonally to the first axis and to the second axis and generally through a wing of the aircraft. Body to local level accelerations module 126 multiplies body-axis accelerations 14 (i.e., a three-element vector of accelerations) by direction-cosine matrix DC to transform body-axis accelerations 14 from the body-axis reference frame to the local level reference frame defined by three mutually-orthogonal axes, a first of the three axes directed in a North direction, a second of the three axes directed in an East direction, and a third of the three axes directed orthogonally to the first axis and to the second axis toward the center of the Earth. Body to local level accelerations module 126 extracts the component of body-axis accelerations 14 in the local level reference frame directed along the third axis toward the center of the Earth and provides the extracted component to integrator 132 as vertical acceleration A_(vert).

As illustrated in FIG. 6, complementary filter 128 includes differentiator 130, integrator 132, low-pass filter 134, high-pass filter 136, and summing junction 138. Differentiator 130 receives pressure altitude 39 as input and provides pressure-based altitude rate dh/dt representing the derivative of pressure altitude 39 with respect to time as output to low-pass filter 134. In addition, pressure-based altitude rate dh/dt is provided to integrator 132 as an initial condition during a first execution of altitude rate blending module 23 (e.g., on power-up of air data computer 10).

Integrator 132 receives vertical acceleration A_(vert) as input from body to local level accelerations module 126 and provides accelerometer-based vertical velocity V_(vert) representing the integral of vertical acceleration A_(vert) with respect to time. Accelerometer-based vertical velocity V_(vert) is provided to high-pass filter 136 and pressure-based altitude rate dh/dt is provided to low-pass filter 134.

High-pass filter 136 can be a Butterworth filter, an infinite impulse response filter, or other type of filter configured to pass signals with frequencies higher than a cutoff frequency and attenuate signals with frequencies lower than the cutoff frequency to remove low-frequency signal and noise from the input signal. Low-pass filter 134 can be a Butterworth filter, an infinite impulse response filter, or other type of filter configured to pass signals with frequencies lower than a cutoff frequency and attenuate signals with frequencies higher than the cutoff frequency to remove high frequency signal and noise from the input signal. In some examples, low-pass filter 134 and high-pass filter 136 can be matched to have the same cut-off frequency, such that where low-pass filter 134 begins to roll-off in gain, high-pass filter 136 begins to roll-up in gain at the same rate.

High-pass filter 136 filters accelerometer-based vertical velocity V_(vert) to produce filtered accelerometer-based vertical velocity V_(vert-f) that is provided to summing junction 138. Low-pass filter 134 filters pressure-based altitude rate dh/dt to produce filtered pressure-based altitude rate dh/dt-f that is provided to summing junction 138. Summing junction 138 blends (i.e., sums) filtered accelerometer-based vertical velocity V_(vert-f) and filtered pressure-based altitude rate dh/dt-f to produce blended altitude rate 15. Though complementary filter 128 is illustrated in the example of FIG. 6 as including two filters (i.e., low-pass filter 134 and high-pass filter 136) as well as differentiator 130, integrator 132, and summing junction 138, it should be understood that in some examples, differentiator 130, integrator 132, low-pass filter 134, high-pass filter 136, and summing junction 138 can be combined into one multi-input single-output (MISO) filter that takes vertical acceleration A_(vert) and pressure altitude 39 as inputs and produces blended altitude rate 15 as an output.

As described herein, altitude rate blending module 23 utilizes complementary filter 128 to combine low frequency components of pressure-based altitude rate dh/dt (i.e., via low-pass filter 134) with high frequency components of accelerometer-based vertical velocity V_(vert) to produce blended altitude rate 15. As such, altitude rate blending module 23 maintains the accuracy of pressure-based measurements from which pressure altitude 39 is derived and increases a bandwidth of the resulting output via the high frequency components of accelerometer-based vertical velocity V_(vert). Accordingly, altitude rate blending module 23 provides blended altitude rate 15 having accuracy commensurate with pressure-based altitude rate dh/dt and bandwidth (and resulting dynamic response) commensurate with vertical acceleration A_(vert) derived from the high-bandwidth accelerometers 24A-24C.

Discussion of Possible Embodiments

The following are non-exclusive descriptions of possible embodiments of the present invention.

An air data computer configured to be installed on an aircraft includes an inertial sensor assembly, an air data parameter module, an attitude determination module, and an altitude rate blending module. The inertial sensor assembly includes a plurality of accelerometers and a plurality of rate gyroscopes. The air data parameter module is configured to determine a pressure altitude of the aircraft based on measured pressure of airflow about an exterior of the aircraft. The attitude determination module is configured to determine an estimated attitude of the aircraft based on rotational rate sensed by the plurality of rate gyroscopes. The altitude rate blending module is configured to determine a vertical acceleration of the aircraft based on the estimated attitude of the aircraft and acceleration sensed by the plurality of accelerometers, blend the vertical acceleration and the pressure altitude using a complementary filter to produce a blended altitude rate, and output the blended altitude rate

The air data computer of the preceding paragraph can optionally include, additionally and/or alternatively, any one or more of the following features, configurations and/or additional components:

The complementary filter can be configured to: integrate the vertical acceleration to produce an accelerometer-based vertical velocity of the aircraft; differentiate the pressure altitude to produce a pressure-based altitude rate of the aircraft; filter the accelerometer-based vertical velocity to remove low frequency signal and noise to produce a high-pass filtered accelerometer-based vertical velocity; filter the pressure-based altitude rate to remove high frequency signal and noise to produce a low-pass filtered pressure-based altitude rate; and blend the high-pass filtered accelerometer-based vertical velocity and the low-pass filtered pressure-based altitude rate to produce the blended altitude rate of the aircraft.

The complementary filter can be configured to blend the high-pass filtered accelerometer-based vertical velocity and the low-pass filtered pressure-based altitude rate by summing the high-pass filtered accelerometer-based vertical velocity and the low-pass filtered pressure-based altitude rate.

The complementary filter can be a multi-input single-output (MISO) filter that takes the vertical acceleration and the pressure altitude as inputs and produces the blended altitude rate as an output.

The complementary filter can be configured to filter the accelerometer-based vertical velocity to remove the low frequency signal and noise using a high-pass filter. The complementary filter can be configured to filter the pressure-based altitude rate to remove the high frequency signal and noise using a low-pass filter.

A cutoff frequency of the high-pass filter can match a cut-off frequency of the low-pass filter.

The altitude rate blending module can be configured to determine the vertical acceleration of the aircraft based on the estimated attitude of the aircraft and the acceleration sensed by the plurality of accelerometers by multiplying the acceleration sensed by the plurality of accelerometers and a direction-cosine matrix having direction angles corresponding to roll and pitch of the aircraft.

The plurality of accelerometers can include three accelerometers, each configured to sense acceleration along one of three mutually-orthogonal axes. The plurality of rate gyroscopes can include three rate gyroscopes, each configured to sense rotational rate along one of the three mutually-orthogonal axes.

The air data parameter module can be further configured to determine a true airspeed of the aircraft based on the measured pressure of airflow about the exterior of the aircraft. The air data computer can further include an inertial compensation and correction module and a Kalman estimator module. The Kalman estimator module can be configured to: determine a change in integrated acceleration of the air data computer over a time interval based on acceleration sensed by the plurality of accelerometers and rotational rate sensed by the plurality of rate gyroscopes; determine a set of error correction values based on a difference between the change in the integrated acceleration of the air data computer and a change in the true airspeed of the air data computer; and provide the set of error correction values to the inertial sensor compensation and correction module. The inertial sensor compensation and correction module can be further configured to: apply the set of error correction values to each of the acceleration sensed by the plurality of accelerometers and the rotational rate sensed by the plurality of rate gyroscopes to produce an error-corrected acceleration and error-corrected rotational rate; provide the error-corrected rotational rate to the attitude determination module for determination of the estimated attitude of the aircraft; and provide the error-corrected acceleration to the altitude rate blending module for determination of the vertical acceleration of the aircraft.

The Kalman estimator module can be configured to determine the set of error correction values via an extended Kalman filter that utilizes the difference between the change in the integrated acceleration of the air data computer and the change in the true airspeed of the air data computer as input and produces the set of error correction values as output.

A method includes sensing acceleration of an air data computer configured to be installed on an aircraft along a plurality of axes via a plurality of accelerometers of an inertial sensor assembly of the air data computer. The method further includes sensing rotational rate of the air data computer along the plurality of axes via a plurality of rate gyroscopes of the inertial sensor assembly. The method further includes determining a pressure altitude of the aircraft based on measured pressure of airflow about an exterior of the aircraft, determining an estimated attitude of the aircraft based on the rotational rate sensed by the plurality of rate gyroscopes, and determining a vertical acceleration of the aircraft based on the estimated attitude of the aircraft and the acceleration sensed by the plurality of accelerometers. The method further includes blending the vertical acceleration and the pressure altitude using a complementary filter to produce a blended altitude rate, and outputting the blended altitude rate.

The method of the preceding paragraph can optionally include, additionally and/or alternatively, any one or more of the following features, configurations, operations and/or additional components:

Blending the vertical acceleration and the pressure altitude using the complementary filter can include: integrating the vertical acceleration to produce an accelerometer-based vertical velocity of the aircraft; differentiating the pressure altitude to produce a pressure-based altitude rate of the aircraft; filtering the accelerometer-based vertical velocity to remove low frequency signal and noise to produce a high-pass filtered accelerometer-based vertical velocity; filtering the pressure-based altitude rate to remove high frequency signal and noise to produce a low-pass filtered pressure-based altitude rate; and blending the high-pass filtered accelerometer-based vertical velocity and the low-pass filtered pressure-based altitude rate to produce the blended altitude rate of the aircraft.

Blending the high-pass filtered accelerometer-based vertical velocity and the low-pass filtered pressure-based altitude rate can include summing the high-pass filtered accelerometer-based vertical velocity and the low-pass filtered pressure-based altitude rate.

Integrating the vertical acceleration, differentiating the pressure altitude, filtering the accelerometer-based vertical velocity, filtering the pressure-based altitude rate, and blending the high-pass filtered accelerometer-based vertical velocity and the low-pass filtered pressure-based altitude rate can be performed using a multi-input single-output (MISO) filter that takes the vertical acceleration and the pressure altitude as inputs and produces the blended altitude rate as an output.

Filtering the accelerometer-based vertical velocity to remove the low frequency signal and noise can include filtering the accelerometer-based vertical velocity using a high-pass filter. Filtering the pressure-based altitude rate to remove the high frequency signal and noise can include filtering the pressure-based altitude rate using a low-pass filter.

A cutoff frequency of the high-pass filter can match a cut-off frequency of the low-pass filter.

Determining the vertical acceleration of the aircraft based on the estimated attitude of the aircraft and the acceleration sensed by the plurality of accelerometers can include multiplying the acceleration sensed by the plurality of accelerometers and a direction-cosine matrix having direction angles corresponding to roll and pitch of the aircraft.

Sensing the acceleration along the plurality of axes via the plurality of accelerometers can include sensing the acceleration along three mutually-orthogonal axes via three accelerometers. Sensing the rotational rate along the plurality of axes via the plurality of rate gyroscopes can include sensing the rotational rate along the three mutually-orthogonal axes via three rate gyroscopes.

The method can further include: determining a true airspeed of the aircraft based on the measured pressure of airflow about the exterior of the aircraft; determining a change in integrated acceleration of the air data computer over a time interval based on the acceleration sensed by the plurality of accelerometers and the rotational rate sensed by the plurality of rate gyroscopes; determining a set of error correction values based on a difference between the change in the integrated acceleration of the air data computer and a change in the true airspeed of the air data computer; and applying the set of error correction values to each of the acceleration sensed by the plurality of accelerometers and the rotational rate sensed by the plurality of rate gyroscopes.

Determining the set of error correction values can include determining the set of error correction values via an extended Kalman filter that utilizes the difference between the change in the integrated acceleration of the air data computer and the change in the true airspeed of the air data computer as input and produces the set of error correction values as output.

While the invention has been described with reference to an exemplary embodiment(s), it will be understood by those skilled in the art that various changes may be made and equivalents may be substituted for elements thereof without departing from the scope of the invention. In addition, many modifications may be made to adapt a particular situation or material to the teachings of the invention without departing from the essential scope thereof. Therefore, it is intended that the invention not be limited to the particular embodiment(s) disclosed, but that the invention will include all embodiments falling within the scope of the appended claims. 

The invention claimed is:
 1. An air data computer configured to be installed on an aircraft, the air data computer comprising: an inertial sensor assembly comprising a plurality of accelerometers and a plurality of rate gyroscopes; an air data parameter module configured to determine a pressure altitude of the aircraft based on measured pressure of airflow about an exterior of the aircraft; an attitude determination module configured to determine an estimated attitude of the aircraft based on rotational rate sensed by the plurality of rate gyroscopes; and an altitude rate blending module configured to: determine a vertical acceleration of the aircraft based on the estimated attitude of the aircraft and acceleration sensed by the plurality of accelerometers; perform a mathematical integration of the vertical acceleration to produce an accelerometer-based vertical velocity of the aircraft; perform a mathematical differentiation of the pressure altitude to produce a pressure-based altitude rate of the aircraft; filter, via a complementary filter, the accelerometer-based vertical velocity to remove low frequency signal and noise to produce a high-pass filtered accelerometer-based vertical velocity; filter, via the complementary filter, the pressure-based altitude rate to remove high frequency signal and noise to produce a low-pass filtered pressure-based altitude rate; and blend the high-pass filtered accelerometer-based vertical velocity and the low-pass filtered pressure-based altitude rate to produce the blended altitude rate of the aircraft; and output the blended altitude rate.
 2. The air data computer of claim 1, wherein the complementary filter is configured to blend the high-pass filtered accelerometer-based vertical velocity and the low-pass filtered pressure-based altitude rate by summing the high-pass filtered accelerometer-based vertical velocity and the low-pass filtered pressure-based altitude rate.
 3. The air data computer of claim 1, wherein the complementary filter is a multi-input single-output (MISO) filter that takes the vertical acceleration and the pressure altitude as inputs and produces the blended altitude rate as an output.
 4. The air data computer of claim 1, wherein the complementary filter is configured to filter the accelerometer-based vertical velocity to remove the low frequency signal and noise using a high-pass filter; and wherein the complementary filter is configured to filter the pressure-based altitude rate to remove the high frequency signal and noise using a low-pass filter.
 5. The air data computer of claim 4, wherein a cutoff frequency of the high-pass filter matches a cut-off frequency of the low-pass filter.
 6. The air data computer of claim 1, wherein the altitude rate blending module is configured to determine the vertical acceleration of the aircraft based on the estimated attitude of the aircraft and the acceleration sensed by the plurality of accelerometers by multiplying the acceleration sensed by the plurality of accelerometers and a direction-cosine matrix having direction angles corresponding to roll and pitch of the aircraft.
 7. The air data computer of claim 1, wherein the plurality of accelerometers comprises three accelerometers, each configured to sense acceleration along one of three mutually-orthogonal axes; and wherein the plurality of rate gyroscopes comprises three rate gyroscopes, each configured to sense rotational rate along one of the three mutually-orthogonal axes.
 8. The air data computer of claim 1, wherein the air data parameter module is further configured to determine a true airspeed of the aircraft based on the measured pressure of airflow about the exterior of the aircraft, the air data computer further comprising: an inertial compensation and correction module; and a Kalman estimator module configured to: determine a change in integrated acceleration of the air data computer over a time interval based on acceleration sensed by the plurality of accelerometers and rotational rate sensed by the plurality of rate gyroscopes; determine a set of error correction values based on a difference between the change in the integrated acceleration of the air data computer and a change in the true airspeed of the air data computer; and provide the set of error correction values to the inertial sensor compensation and correction module; wherein the inertial sensor compensation and correction module is further configured to: apply the set of error correction values to each of the acceleration sensed by the plurality of accelerometers and the rotational rate sensed by the plurality of rate gyroscopes to produce an error-corrected acceleration and error-corrected rotational rate; provide the error-corrected rotational rate to the attitude determination module for determination of the estimated attitude of the aircraft; and provide the error-corrected acceleration to the altitude rate blending module for determination of the vertical acceleration of the aircraft.
 9. The air data computer of claim 8, wherein the Kalman estimator module is configured to determine the set of error correction values via an ex tended Kalman filter that utilizes the difference between the change in the integrated acceleration of the air data computer and the change in the true airspeed of the air data computer as input and produces the set of error correction values as output.
 10. The method of claim 8, wherein determining the set of error correction values comprises determining the set of error correction values via an extended Kalman filter that utilizes the difference between the change in the integrated acceleration of the air data computer and the change in the true airspeed of the air data computer as input and produces the set of error correction values as output.
 11. A method comprising: sensing acceleration of an air data computer configured to be installed on an aircraft along a plurality of axes via a plurality of accelerometers of an inertial sensor assembly of the air data computer; sensing rotational rate of the air data computer along the plurality of axes via a plurality of rate gyroscopes of the inertial sensor assembly; determining a pressure altitude of the aircraft based on measured pressure of airflow about an exterior of the aircraft; determining an estimated attitude of the aircraft based on the error-corrected rotational rate; determining a vertical acceleration of the aircraft based on the estimated attitude of the aircraft and the error-corrected acceleration; performing a mathematical integration of the vertical acceleration to produce an accelerometer-based vertical velocity of the aircraft; performing a mathematical differentiation of the pressure altitude to produce a pressure-based altitude rate of the aircraft; filtering, via a complementary filter, the accelerometer-based vertical velocity to remove low frequency signal and noise to produce a high-pass filtered accelerometer-based vertical velocity; filtering, via a complementary filter, the pressure-based altitude rate to remove high frequency signal and noise to produce a low-pass filtered pressure-based altitude rate; and blending the high-pass filtered accelerometer-based vertical velocity and the low-pass filtered pressure-based altitude rate to produce the blended altitude rate of the aircraft; and outputting the blended altitude rate.
 12. The method of claim 11, wherein blending the high-pass filtered accelerometer-based vertical velocity and the low-pass filtered pressure-based altitude rate comprises summing the high-pass filtered accelerometer-based vertical velocity and the low-pass filtered pressure-based altitude rate.
 13. The method of claim 11, wherein integrating the vertical acceleration, differentiating the pressure altitude, filtering the accelerometer-based vertical velocity, filtering the pressure-based altitude rate, and blending the high-pass filtered accelerometer-based vertical velocity and the low-pass filtered pressure-based altitude rate are performed using a multi-input single-output (MISO) filter that takes the vertical acceleration and the pressure altitude as inputs and produces the blended altitude rate as an output.
 14. The method of claim 11, wherein filtering the accelerometer-based vertical velocity to remove the low frequency signal and noise comprises filtering the accelerometer-based vertical velocity using a high-pass filter; and wherein filtering the pressure-based altitude rate to remove the high frequency signal and noise comprises filtering the pressure-based altitude rate using a low-pass filter.
 15. The method of claim 14, wherein a cutoff frequency of the high-pass filter matches a cut-off frequency of the low-pass filter.
 16. The method of claim 11, wherein determining the vertical acceleration of the aircraft based on the estimated attitude of the aircraft and the acceleration sensed by the plurality of accelerometers comprises multiplying the acceleration sensed by the plurality of accelerometers and a direction-cosine matrix having direction angles corresponding to roll and pitch of the aircraft.
 17. The method of claim 11, wherein sensing the acceleration along the plurality of axes via the plurality of accelerometers comprises sensing the acceleration along three mutually-orthogonal axes via three accelerometers; and wherein sensing the rotational rate along the plurality of axes via the plurality of rate gyroscopes comprises sensing the rotational rate along the three mutually-orthogonal axes via three rate gyroscopes.
 18. The method of claim 11, further comprising: determining a true airspeed of the aircraft based on the measured pressure of airflow about the exterior of the aircraft; determining a change in integrated acceleration of the air data computer over a time interval based on the acceleration sensed by the plurality of accelerometers and the rotational rate sensed by the plurality of rate gyroscopes; determining a set of error correction values based on a difference between the change in the integrated acceleration of the air data computer and a change in the true airspeed of the air data computer; and applying the set of error correction values to each of the acceleration sensed by the plurality of accelerometers and the rotational rate sensed by the plurality of rate gyroscopes. 